LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

L C L S C O N C E P T U A L D E S I G N R E P O R T
22 D.T. Palmer et al., in Proc. of the 1995 Particle Accelerator Conf. (1995), p. 982. In this reference it is
pointed out that the dipole emittance term has been suppressed by an order of magnitude to the level of
0.1 µm, implying that in the unsymmetrized case the dipole emittance term would be 1 µm. See also
B. Dwersteg et al., “rf gun design for the TESLA VUV free electron laser,” Nucl. Instrum. and Meth.
A 393 (1997) 93.
23 E.L. Ginzton, Microwave Measurements, McGraw-Hill (1957), p. 295.
24 X.-J. Wang et al., “Design studies for the LCLS 120 Hz rf gun,” Informal Report BNL-67922 (Dec.
2000).
25 M. Uesaka (U. Tokyo) and M. Kando (JAERI Advanced Photon Research Center), private
communication (11/00).
26 J. Schmerge, “120 Hz RF gun operation,” draft of internal SLAC technical report (6/00).
27 H. Braun et al., “Results from the CLIC Test Facility,” in Proc. of the 5 th European Particle
Accelerator Conf., (1996), p. 44.
28 T. Srinivasan-Rao et al., J. Appl. Phys. 69 (1991) 3291.
29 P. Davis et al., in Proc. of the 1993 Particle Accelerator Conf., p. 2976.
30 E. Chevallay et al., Nucl. Instrum. and Meth. A 340 (1994) 146.
31 G. Mulhollan, "Common Sense Copper and RF Guns," LCLS-TN-99-9 (July 1999).
32 D. Reis, Ph.D. Thesis, Univ. Rochester, Dept. of Physics and Astronomy, June 1999, UR-1573, pp.
130-131.
33 D. Reis et al., Nucl. Instrum. and Meth. A 429 (1999) 341.
34 D.T. Palmer, SLAC, private communication (1997).
35 X.-J. Wang et al., "FEL technologies R&D and SASE gain enhancement observation at the BNL
ATF," in Proc. of the 2000 European Particle Accelerator Conf., p. 779.
36 The gain per pass in Ti:sapphire amplifiers is sufficient to get from 1 nJ to a few mJ in eight (8) passes.
For example, see S. Backus et al., Opt. Lett. 20 (1995) 2000.
35-1 J.A. Hoffnagle and C.M. Jefferson, Appl. Opt. 39 (2000) 5488.
37 P. Maine et al., IEEE J. Quantum Electron. QE-24 (1988) 398.
38 A.M. Weiner et al., J. Opt. Soc. B 5 (1988) 1563.
39 A.M. Weiner et al., Opt. Lett. 15 (1990) 326; A.M. Weiner, Rev. Sci. Instrum. 71 (2000) 1929.
40 ShapeShifter spatial light modulator, Meadowlark Optics, Frederick, CO.
41 B.M. Van Wonterghem et al., Proc. of the Conference on Laser Coherence Control, in SPIE 1870
(1993), p. 64.
42 J.A. Hoffnagle and C.M. Jefferson, Appl. Opt. 39 (2000) 5488.
43 R.S. Craxton, Opt. Commun. 34 (1980) 474.
44 For ultrafast laser pulses, the effects of group velocity walkoff and nonlinear phase effects must be
considered when designing the conversion stage.
45 D.A. Reis, Ph.D. Thesis, Univ. Rochester, Dept. of Physics and Astronomy, June 1999, UR-1573, pp.
23 and 131.
46 P. Davis et al., Proc. 1993 Particle Accelerator Conf., p. 2976.
47 H.-S. Albrecht et al., Appl. Opt. 32 (1993) 6659.
48 D.J. Kane and R. Trebino, Opt. Lett. 18 (1993) 823.
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